This paper classifies all finitely generated projective modules over quantum odd-dimensional spheres and explicitly identifies quantum line bundles as concrete projections, advancing the understanding of quantum homogeneous spaces.
Contribution
It provides a complete classification of projective modules over quantum spheres and explicitly constructs quantum line bundles as concrete projections.
Findings
01
Complete classification of projective modules over quantum spheres
02
Explicit identification of quantum line bundles as projections
03
Enhanced understanding of quantum homogeneous space structures
Abstract
We give a complete classification of isomorphism classes of finitely generated projective modules, or equivalently, unitary equivalence classes of projections, over the C*-algebra C(Sq2n+1) of the quantum homogeneous sphere Sq2n+1. Then we explicitly identify as concrete elementary projections the quantum line bundles Lk over the quantum complex projective space CPqn associated with the quantum Hopf principal U(1)-bundle Sq2n+1→CPqn.
P_{j,k}:=\left\{\begin{array}[c]{lll}1_{\mathbb{T}}\otimes\left(\left(\otimes^{j-1}P_{1}\right)\otimes P_{k}\otimes\left(\otimes^{n-j}I\right)\right)\in C\left(\mathbb{T}\right)\otimes\left(\mathcal{K}^{+}\right)^{\otimes n},&\text{if }&k>0\text{ and }1\leq j\leq n\\
1_{\mathbb{T}}\otimes\left(\boxplus^{k}I^{\otimes n}\right)\equiv 1_{\mathbb{T}}\otimes\left(\boxplus^{k}\left(\otimes^{n}I\right)\right)\in M_{k}\left(C\left(\mathbb{T}\right)\otimes\left(\mathcal{K}^{+}\right)^{\otimes n}\right),&\text{if }&k\geq 0\text{ and }j=0\end{array}\right.
P_{j,k}:=\left\{\begin{array}[c]{lll}1_{\mathbb{T}}\otimes\left(\left(\otimes^{j-1}P_{1}\right)\otimes P_{k}\otimes\left(\otimes^{n-j}I\right)\right)\in C\left(\mathbb{T}\right)\otimes\left(\mathcal{K}^{+}\right)^{\otimes n},&\text{if }&k>0\text{ and }1\leq j\leq n\\
1_{\mathbb{T}}\otimes\left(\boxplus^{k}I^{\otimes n}\right)\equiv 1_{\mathbb{T}}\otimes\left(\boxplus^{k}\left(\otimes^{n}I\right)\right)\in M_{k}\left(C\left(\mathbb{T}\right)\otimes\left(\mathcal{K}^{+}\right)^{\otimes n}\right),&\text{if }&k\geq 0\text{ and }j=0\end{array}\right.
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Full text
Projections over Quantum Homogeneous Odd-dimensional Spheres††thanks: This work
was partially supported by the grant H2020-MSCA-RISE-2015-691246-QUANTUM
DYNAMICS and the Polish government grant 3542/H2020/2016/2.
Albert Jeu-Liang Sheu
Department of Mathematics, University of Kansas, Lawrence, KS 66045,
U. S. A.
We give a complete classification of isomorphism classes of finitely generated
projective modules, or equivalently, unitary equivalence classes of
projections, over the C*-algebra C(Sq2n+1) of
the quantum homogeneous sphere Sq2n+1. Then we explicitly
identify as concrete elementary projections the quantum line bundles Lk
over the quantum complex projective space CPqn associated
with the quantum Hopf principal U(1)-bundle Sq2n+1→CPqn.
1 Introduction
In the theory of quantum/noncommutative geometry popularized by Connes
[6], C*-algebras are often viewed as the algebra C(Xq) of continuous functions on a virtual quantum space Xq,
and finitely generated projective (left) C(Xq)-module
Γ(Eq) are viewed as virtual vector bundles over the
quantum space Xq. The former viewpoint is motivated by Gelfand’s Theorem
identifying all commutative C*-algebras as exactly function algebras
C0(X) for locally compact Hausdorff spaces X, while the
latter is motivated by Swan’s Theorem [27] characterizing all finitely
generated projective C(X)-modules for a compact Hausdorff
space X as exactly the spaces Γ(E) of continuous
cross-sections of vector bundles E over X.
As spheres and projective spaces provide fundamentally important examples for
the classical study of topology and geometry, quantum versions of spheres and
projective spaces have been developed and provide important examples for the
study of quantum geometry. In particular, from the quantum group viewpoint
[9, 30, 31], Soibelman, Vaksman, Meyer and others
[29, 14, 15, 24] introduced and studied the homogeneous
odd-dimensional quantum sphere Sq2n+1 and the associated
quantum complex projective space CPqn, and from the
multipullback viewpoint, Hajac and his collaborators including Baum, Kaygun,
Matthes, Nest, Pask, Sims, Szymański, Zieliński, and others
[12, 11, 13] developed and studied the multipullback
odd-dimensional quantum sphere SH2n+1 and the associated
quantum complex projective space Pn(T).
As in the classical situation, the above mentioned quantum odd-dimensional
spheres and their associated quantum complex projective spaces provide a
quantum Hopf principal U(1)-bundle, from which some
associated quantum line bundles Lk, or rank-one projective modules over
the quantum algebra of the complex projective space, for k∈Z are
constructed [14, 2, 12, 13].
It is well known that classifying up to isomorphism all vector bundles over a
space X in the classical case or finitely generated (left) projective
modules over a C*-algebra C(Xq) in the quantum case is an
interesting but difficulty task. A major challenge in such classification is
the so-called cancellation problem [18, 19] which deals with
determining whether the stable isomorphism between such objects determined by
K-theoretic analysis can imply their isomorphism.
In this paper, we use the powerful groupoid approach to C*-algebras initiated
by Renault [17] and popularized by Curto, Muhly, and Renault
[7, 16] to study the C*-algebra structures of C(Sq2n+1) and C(CPqn).
In this framework, we work to get a complete classification of projections
over C(Sq2n+1) up to equivalence, extending
the result of Bach [4], and determine the canonical monoid structure on
the collection of all equivalence classes of projections over C(Sq2n+1) with the diagonal sum ⊞ as its binary
operation. In particular, we get infinitely many inequivalent projections over
C(Sq2n+1) which are stably equivalent over
C(Sq2n+1), showing that the cancellation
property does not hold for projections over C(Sq2n+1) as elaborated in Corollary 1. Then we proceed to present a
set of elementary projections that freely generate K0(C(CPqn)) and represent the line bundles Lk
over CPqn by concrete ⊞-sum of elementary
projections. We mention that a similar study has been carried out for the
multipullback quantum spheres SH2n+1 and the associated
projective space Pn(T) in the paper
[26, 25], and an interesting geometric study via Milnor
construction is presented by Farsi, Hajac, Maszczyk, and Zieliński in
[10] for C(P2(T)).
Among works in the literature related to our topic here, we mention that the
graph C*-algebra of any row-finite graph, including C(Sq2n+1), satisfies the so-called stable weak cancellation
property [1], and that a “geometric” realization of generators of K0(C(CPqn)) using Milnor connecting
homomorphism is found in [3], beside the geometric study of quantum
line bundles over CPqn in [2]. It would be of
interest to take a close look at potential underlying connections between
these works and ours. (The author thanks the referee for relevant references
to the literature.)
The author would like to thank Prof. Dabrowski for hosting his visit to SISSA,
Trieste, Italy in the spring of 2018, and also thank him and Prof. Landi for
useful discussions and questions about quantum odd-dimensional spheres and
quantum complex projective spaces.
2 Preliminary notations
In this paper, we use freely the basic techniques and manipulations for
K-theory of C*-algebras, or more generally, Banach algebras, found in
[5, 28]. Commonly widely used notations like M∞(A), GL∞(A), unitization
A+, diagonal sum P⊞Q of elements P,Q∈M∞(A), the identity component G0 of a
topological group G, the positive cone K0(A)+ of K0(A), B(H), K(H), and others
will not be explained in details here, and we refer to the notations section
in [26] for any need of further clarification.
By a projection (or an idempotent) over a C*-algebra A, we mean a
projection (or an idempotent) in the algebra M∞(A) of all finite matrices with entries in A. Two
projections (or idempotents) P,Q∈M∞(A)
are called equivalent over A, denoted as P∼AQ,
if there is an invertible U∈GL∞(A) such
that UPU−1=Q.
We recall that the mapping P↦AnP induces a bijective
correspondence between the equivalence (respectively, the stable equivalence)
classes of idempotents over A and the isomorphism (respectively,
the stable isomorphism) classes of finitely generated projective modules over
A [5], where by a module over A, we mean a
left A-module, unless otherwise specified.
We also recall that the K0-group K0(A)
classifies idempotents over A up to stable equivalence. The
classification of idempotents up to equivalence, appearing as the so-called
cancellation problem, was popularized by Rieffel’s pioneering work
[18, 19] and is in general an interesting but difficult question.
For a C*-algebra homomorphism h:A→B, we use
the same symbol h, instead of the more formal symbol M∞(h), to denote the algebra homomorphism M∞(A)→M∞(B) that
applies h to each entry of any matrix in M∞(A).
The set of all equivalence classes of idempotents, or equivalently, all
unitary equivalence classes of projections, over a C*-algebra A is
an abelian monoid P(A) with its binary
operation provided by the diagonal sum ⊞.
In the following, we use the notations Z≥k:={n∈Z∣n≥k} and Z≥:=Z≥0.
In particular, N=Z≥1. We use I to denote the
identity operator canonically contained in K+⊂B(ℓ2(Z≥)), and
[TABLE]
to denote the standard m×m identity matrix in Mm(C)⊂K for any integer m≥0 (with
M0(C)=0 and P0=0 understood). We also use
the notation
[TABLE]
for integers m>0, and take symbolically P−0≡I−P0=I=P0.
This should not cause any trouble since we will not formally add up the
subscripts of these P-projections without necessary clarification.
3 Quantum spaces as groupoid C*-algebras
In the following, we work with some concrete r-discrete (or étale)
groupoids and use them to analyze and encode important structures of quantum
Sq2n+1 and quantum CPqn in the context of
groupoid C*-algebras. This groupoid approach to C*-algebras was popularized by
the work of Curto, Muhly, and Renault [7, 16, 20] and shown to be
useful in the study of quantum homogeneous spaces
[22, 21, 23, 24]. We refer readers to Renault’s pioneering
book [17] for the fundamental theory of groupoid C*-algebras.
We denote by Z:=Z∪{+∞}
the discrete space Z with a point +∞≡∞ canonically
adjoined as a limit point at the positive end, and take Z≥:≡{n∈Z∣n≥0}⊂Z.
(We could also take Z to be the one-point
compactification of the discrete space Z in this paper since
essentially we work only with groupoids restricted to a positive cone of their
unit spaces.) The group Z acts by homeomorphisms on Z in the canonical way, namely, by translations on Z
while fixing the point ∞. More generally, the group Zn
acts on Zn componentwise in such a way. Let
Fn:=Z×(Zn⋉Zn)∣Z≥n
with n≥1 be the direct product of the group Z and the
transformation groupoid Zn⋉Zn
restricted to the positive “cone” Z≥n, where Z≥ is
the closure Z≥∪{∞} of Z≥ in Z. (Later we also use Z≥ to denote this positive part Z≥ of
Z.)
As shown in [23], C(Sq2n+1)≃C∗(Fn), where Fn is a
subquotient groupoid of Fn, namely, Fn:=Fn/∼ for the subgroupoid
[TABLE]
[TABLE]
of Fn, where ∼ is the equivalence relation generated by
[TABLE]
for all (z,x,w) with wi=∞ for an 1≤i≤n.
The unit space of Fn is Z:=Z≥n/∼ where Z≥n is the unit space of
Fn⊂Fn embedded in
Fn as the ∼-invariant subset {0}×{0}×Z≥n.
Let πn denote the faithful -representation of the groupoid C-algebra
C∗(Fn) canonically constructed on the
Hilbert space ℓ2(Z×Z≥n)=ℓ2(Z)⊗ℓ2(Z≥n) built from the open dense orbit Z≥n in the
unit space Z of Fn. For practical purposes, we often
identify C∗(Fn) with the concrete
operator algebra πn(C∗(Fn)) without making explicit distinction. Note that by restricting
Fn to the open subset Z≥n, we get the
groupoid Fn∣Z≥n≅Z×((Zn⋉Zn)∣Z≥n) with
[TABLE]
under the representation πn, where C∗(Z)≅C(T) acts on ℓ2(Z)≅L2(T) by multiplication operators,
and hence C(T)⊗K(ℓ2(Z≥n)) can be viewed as a closed
ideal of πn(C∗(Fn))≡C∗(Fn).
Note that the Z-component of Fn≡Z×(Zn⋉Zn)∣Z≥n gives a grading on C∗(Fn), decomposing it into (a completion of) a direct sum
of some subspaces index by Z. More precisely,
Fn is the union of the pairwise disjoint closed
and open sets
[TABLE]
with k∈Z which are invariant under the equivalence relation
∼, so F≡Fn/∼ is the union
of the pairwise disjoint closed and open sets
[TABLE]
and hence C∗(Fn) is the closure of the
(algebraic) direct sum ⊕k∈ZCc(Fn)k where Cc(Fn)k:=Cc((Fn)k). In fact, the
groupoid character [(k,x,w)]∈Fn↦tk∈T for any fixed t∈T≡U(1) defines an isometric -automorphism of L1(Fn) and hence a C-algebra automorphism ρ(t) of C∗(Fn), sending
δ[(k,x,w)] to tkδ[(k,x,w)]. Clearly ρ:t↦ρ(t) defines a U(1)-action on C∗(Fn). The degree-k spectral subspace C∗(Fn)k of C∗(Fn)
under the action ρ, i.e. the set consisting of all elements a∈C∗(Fn) with (ρ(t))(a)=tka for all t∈T, is a closed
linear subspace of C∗(Fn) containing
Cc(Fn)k. Clearly C∗(Fn)k∩C∗(Fn)k′=0 for any k=k′. The integration operator
[TABLE]
is a well-defined continuous projection onto C∗(Fn)k and eliminates C∗(Fn)l for all l=k, where T is endowed with the standard Haar
measure. Indeed for any s∈T,
[TABLE]
[TABLE]
and for any b∈C∗(Fn)l,
[TABLE]
So Λk’s are mutually orthogonal projections in the sense that
Λk∘Λl=δklΛk. With the (algebraic) sum
∑k∈ZCc(Fn)k clearly
dense in C∗(Fn) and Cc(Fn)k⊂C∗(Fn)k, we see that Cc(Fn)k=C∗(Fn)k by applying the projection
operator Λk to any sequence in ∑l∈ZCc(Fn)l converging to an element of C∗(Fn)k. Furthermore we note that clearly Cc(Fn)kCc(Fn)l⊂Cc(Fn)k+l and C∗(Fn)kC∗(Fn)l⊂C∗(Fn)k+l for all
k,l∈Z, i.e. Cc(Fn) and
C∗(Fn) are graded algebras (up to completion).
Recall that the group U(1)≡T acts on C(Sq2n+1) by sending the standard generators
un+1,m∈C(SUq(n+1)), 1≤m≤n+1, of C(Sq2n+1) to tun+1,m for each
group element t∈T⊂C. This U(1)-action, denoted as τt for t∈T, decomposes C(Sq2n+1) into spectral subspaces C(Sq2n+1)k of degree k∈Z consisting of
elements a∈C(Sq2n+1) satisfying τt(a)=tka for all t∈T. Each un+1,m is
in the degree-1 spectral subspace C(Sq2n+1)1. On the other hand, under the identification of C(Sq2n+1) with C∗(Fn)
established in the work of [22, 23], each un+1,m faithfully
represented as tn+1⊗γ⊗n+1−m⊗α∗⊗1⊗m−2 is identified with an element in Cc(Fn)1=C∗(Fn)1. So the grading on C∗(Fn) by C∗(Fn)k coincides
with the grading on C(Sq2n+1) by C(Sq2n+1)k, i.e. C(Sq2n+1)k=C∗(Fn)k.
The degree-[math] spectral subspace C(Sq2n+1)0, or equivalently, the U(1)-invariant subalgebra (C(Sq2n+1))U(1) of
C(Sq2n+1) can be naturally called the algebra
of quantum CPn, denoted as C(CPqn). The embedding C(CPqn)⊂C(Sq2n+1)≡C∗(Fn), or virtually the quantum quotient map Sq2n+1→CPqn, is a quantum analogue of the Hopf principal U(1)-bundle S2n+1→CPn. Furthermore
the degree-k spectral subspaces C(Sq2n+1)k≡C∗(Fn)k become the quantum
line bundles, denoted Lk, over CPqn associated with the
quantum principal U(1)-bundle Sq2n+1→CPqn. Note that in the context of groupoid
C*-algebras, C(CPqn)≡C(Sq2n+1)0 is canonically identified with the
groupoid C*-algebra C∗((Fn)0) where (Fn)0 is clearly an
open and closed subgroupoid of Fn. It is easy to see that the
unit space of (Fn)0⊂Fn
is the same unit space Z≡Z≥n/∼ that
Fn has.
On the other hand, the quantum complex projective space U(n)q\SU(n+1)q has been formulated and studied by
researchers from the viewpoint of quantum homogeneous space [15]. The
author showed in [24] that such a quantum space can be concretely
realized by the C*-subalgebra generated by un+1,i∗un+1,j with
1≤i,j≤n+1 in C(Sq2n+1), and then
identified this C*-algebra with the groupoid C*-algebra C∗(Tn) of the subquotient groupoid Tn:=Tn/∼ of Zn⋉Zn∣Z≥n, where
[TABLE]
[TABLE]
is a subgroupoid of Zn×Zn∣Z≥n and ∼ is the equivalence
relation generated by
[TABLE]
for all (x,w) with wi=∞ for an 1≤i≤n. It is easy to see
that [(0,x,w)]∈(Fn)0↦[(x,w)]∈Tn is a well-defined homeomorphic groupoid isomorphism, and
hence C∗(Tn)≅C∗((Fn)0). So the quantum homogeneous space U(n)q\SU(n+1)q coincides with the
quantum complex projective space CPqn defined above, and the
results obtained in [24] are valid for our study of the quantum
complex projective space CPqn.
4 Projections over C(Sq2n+1)
In [24], taking the groupoid C*-algebra approach, we established an
inductive family of short exact sequences of C*-algebras
[TABLE]
However for the purpose of classification of projections over C(Sq2n+1), it turns out that another inductive family of
short exact sequences constructed below is more convenient.
Under the groupoid monomorphism
[TABLE]
Fn is mapped homeomorphically onto the image
Fn′⊂Fn consisting of
(z,x,w)∈Fn satisfying
[TABLE]
while the equivalence relation ∼ on Fn
remains the same equivalence relation ∼′ on
Fn′ that is generated by
[TABLE]
for all (z,x,w) with wi=∞ for some 1≤i≤n.
So we get a homeomorphic groupoid isomorphism
[TABLE]
Note that the groupoid C*-algebra C∗(Fn′) also has a faithful *-representation πn′
canonically constructed on the Hilbert space ℓ2(Z×Z≥n)=ℓ2(Z)⊗ℓ2(Z≥n) built from the open
dense orbit Z≥n in the unit space of Fn′.
Let m(k) denote (m,...,m)∈Zk. Note that ({∞}×Z≥n−1)/∼={[∞(n)]} is a closed invariant subset
of the unit space Z≡Z≥n/∼ of
Fn such that with a singleton unit space,
[TABLE]
as a group. On the other hand, the complement of {[∞(n)]} in Z is the open invariant
subset O:=(Z≥×Z≥n−1)/∼ such that w1=∞ for all [(z,x,w)]∈Fn∣O and hence in γ([(z,x,w)])=[(z+x1,x,w)], there is no non-trivial condition from the
definition of Fn′/∼′ imposed on
(x1,w1), while the non-trivial conditions from the
definition of Fn′/∼′ imposed on
the other components of γ([(z,x,w)]) match those in defining Fn−1. That is to say,
by rewriting x1,w1 as the first two components of γ([(z,x,w)]), we have a homeomorphic
groupoid isomorphism from Fn∣O onto the groupoid (Z⋉Z)∣Z≥×Fn−1, namely,
[TABLE]
which then induces a C*-algebra isomorphism
[TABLE]
Note that πn′=π0⊗πn−1 on γ∗(C∗(Fn∣O)) where π0:C∗((Z⋉Z)∣Z≥)→K(ℓ2(Z≥)) is the well-known canonical faithful
representation, and the faithful representation
[TABLE]
restricts to an isomorphism C∗(Fn∣O)≅K(ℓ2(Z≥))⊗C(Sq2n−1). So these invariant subsets
{[∞n]} and O give rise to a short
exact sequence
[TABLE]
The set T:={[(z,x,w)]∈Fn:x1=1=−z,x2=...=xn=0} is a compact open subset of
Fn, corresponding to the set {[(0,x,w)]∈Fn′:x=(1,0(n−1))}⊂Fn′ under the
isomorphism γ, and its characteristic function χT∈Cc(Fn)⊂C∗(Fn) determines the operator
[TABLE]
where S is the unilateral shift operator generating the Toeplitz
algebra T with σ(S)=idT for the symbol map σ in the short exact sequence
0→K→T→σC(T)→0. Since the quotient map
η:C∗(Fn)→C∗(Fn∣{[∞n]})≡C∗(Z) restricts χT to
δ1∈Cc(Z)≡Cc(Fn∣{[∞n]})
yielding the function idT∈C(T)≡C∗(Z), we get
[TABLE]
being the sum of K⊗C(Sq2n−1)
and T⊗1C(Sq2n−1), which
coincides with a description of C(Sq2n+1) in
[29].
The above surjective C*-algebra homomorphism C(Sq2n+1)→ηC(T)
facilitates the notion of rank for an equivalence class of idempotent P∈M∞(C(Sq2n+1)) over
C(Sq2n+1), namely, the well-defined classical
rank of the vector bundle over T determined by the idempotent
η(P) over C(T).
The set of equivalence classes of idempotents P∈M∞(C(Sq2n+1)) equipped with the binary operation
⊞ becomes an abelian graded monoid
[TABLE]
where Pr(C(Sq2n+1)) is the set of all (equivalence classes of) idempotents over C(Sq2n+1) of rank r, and
[TABLE]
for r,l≥0. Clearly P0(C(Sq2n+1)) is a submonoid of P(C(Sq2n+1)).
Now we can proceed to classify up to equivalence all projections over
C(Sq2n+1) by induction on n, extending the
result obtained in [4] for the case of n=1.
First we define some standard basic projections
[TABLE]
where I stands for the unit of K+. Note that P0,0=0.
(For the convenience of argument, we also use the symbol Pj,k for the
case of n=0, by taking (K+)⊗0:=C and noting that P0,k=1T⊗(⊞k1)∈Mk(C) for k≥0 makes
sense, while Pj,k with 1≤j≤n does not exist when n=0.)
We note that the basic projection Pj,k with j≥1 is implemented by
the characteristic function χAj,k of the compact open subset
[TABLE]
of Fn under both representations πn and πn′∘γ∗. So each Pj,k with j≥1 is a
projection in C(Sq2n+1). On the other hand,
P0,k=⊞kI~ is the identity projection in Mk(C(Sq2n+1)), where I~ is the
identity element of C(Sq2n+1).
Recall that in the inductive family of short exact sequences
[TABLE]
for C(Sq2n+1) found in [24], the
quotient map μn:C(Sq2n+1)→C(Sq2n−1) is implemented by the restriction
map
[TABLE]
For any n∈N, a projection P over C(Sq2n+1) annihilated by M∞(μn) is a
projection in M∞(C(T)⊗K(ℓ2(Z≥n))) and hence has a well-defined finite operator-rank dn(P)∈Z≥, namely, the rank of the projection operator
P(t)∈M∞(K(ℓ2(Z≥n))), independent of
t∈T. If P is not annihilated by μn, then we assign
dn(P):=∞. Note that dn(P) depends
only on the equivalence class of P over C(Sq2n+1). In the degenerate case of n=0, for a projection P over
C(Sq1)≡C(T), we
define d0(P) to be the finite rank of projection P(t)∈M∞(C), independent of
t∈T.
Now for a projection P over C(Sq2n+1), we
define for 0≤l≤n,
[TABLE]
which depends only on the equivalence class of P over C(Sq2n+1) and gives us a well-defined monoid
homomorphism
[TABLE]
It is easy to verify that
[TABLE]
which shows that these projections Pj,k are mutually inequivalent over
C(Sq2n+1) because Pj,k’s with different
indices (j,k) are distinguished by the collection of
homomorphisms ρ0,ρ1,...,ρn.
Theorem 1. P(C(Sq2n+1)) for n≥0 is the disjoint union of
[TABLE]
containing pairwise distinct [Pj,k]’s indexed by (j,k), and
[TABLE]
and its monoid structure is explicitly determined by that
[TABLE]
So [Pj,k]=0 in K0(C(Sq2n+1)) if and only if 1≤j≤n or j=k=0.
Proof. Knowing that Pj,k are mutually inequivalent, we only need
to show that any projection over C(Sq2n+1) is
equivalent to one of these Pj,k’s and verify the stated monoid structure.
We prove by induction on n≥0.
When n=0, C(Sq2n+1)=C(T) and it is well known from algebraic topology about vector bundles
over T that isomorphism classes of (complex) vector bundles over
T are faithfully represented by trivial vector bundles, i.e.
P0(C(T))={0}≡{[P0,0]} while
Pk(C(T))={[P0,k]} for k>0. Then the statements of this
theorem for n=0 are clearly verified.
Now assume that the statements hold for C(Sq2n−1). We need to show that they also hold for C(Sq2n+1).
Since any complex vector bundle over T is trivial, any idempotent
over C(T) is equivalent to the standard projection
1⊗Pm∈C(T)⊗M∞(C) for some m∈Z≥. So for any nonzero
idempotent P∈M∞(C(Sq2n+1)) over C(Sq2n+1), there is some U∈GL∞(C(T)) such that
[TABLE]
for some m∈Z≥ where I~ is the identity element of
C(Sq2n+1) viewed as the identity element in
(K⊗C(Sq2n−1))+⊂C(Sq2n+1), and hence VPV−1−⊞mI~∈M∞(K⊗C(Sq2n−1)) for any lift V∈GL∞(C(Sq2n+1)) (which exists) of U⊞U−1∈GL∞0(C(T)) along
η. Replacing P by the equivalent VPV−1, we may assume that
P∈(⊞mI~)+Mr−1(K⊗C(Sq2n−1)) for some large r≥m+1.
Now since M∞(C) is dense in K,
there is an idempotent Q∈(⊞mI~)+Mr−1(MN−1(C)⊗C(Sq2n−1)) sufficiently close to and hence
equivalent to P over C(Sq2n+1) for some
large N. So replacing P by Q, we may assume that
[TABLE]
Rearranging the entries of P≡K+⊞mI~∈Mr−1(C(Sq2n+1))⊂Mr(C(Sq2n+1)) via conjugation by the unitary
[TABLE]
[TABLE]
we get the idempotent
[TABLE]
for some idempotent
[TABLE]
which has rank at least m as an idempotent over C(Sq2n−1) since it contains m copies of the identity element
I~′ of C(Sq2n−1) as diagonal
⊞-summands, relocated from the N-th diagonal entry of each of the
m copies of I~ in P.
Now by the induction hypothesis, the idempotent R∈M(r−1)N(C(Sq2n−1)) is equivalent over
C(Sq2n−1) to Pj,k′ (denoting a
standard projection Pj,k over C(Sq2n−1))
with 0≤j≤n−1 and k>0, which is identified with
[TABLE]
i.e. WRW−1=Pj,k′≡Pj+1,k for some invertible W∈MN′(C(Sq2n−1)) with
N′≥(r−1)N. Note that if m>0, then R has a
positive rank as an idempotent over C(Sq2n−1)
and hence j=0. Since
[TABLE]
we get ((⊞mI~)⊞(⊞r−1−m0))⊞R equivalent over C(Sq2n+1) to the projection
[TABLE]
where j=0 if m>0.
If m=0, then clearly P is equivalent over C(Sq2n+1) to Pj+1,k∈K⊗C(Sq2n−1) with j+1>0 and hence is of rank [math]. (We assumed
P\nonzero, so k>0.)
If m∈N and hence j=0, then Pj+1,k=P1,k≡Pk⊗I~′ and we can rearrange entries of ((⊞mI~)⊞(⊞r−1−m0))⊞P1,k via conjugation by the unitary
[TABLE]
[TABLE]
to get P equivalent over C(Sq2n+1) to
[TABLE]
which is of rank m∈N.
So we have proved the description of the sets Pk(C(Sq2n+1)) in the theorem. It remains
to verify the monoid structure of P(C(Sq2n+1)).
By specializing the above analysis for P≡K+⊞mI~ to
the case of K=(⊞m0)⊞Pj+1,k, we have
already established that
[TABLE]
for all m∈N and j+1>0, while [P0,k]⊞[P0,k′]=[P0,k+k′]
is obvious.
On the other hand, by induction hypothesis,
[TABLE]
Now by applying P1⊗⋅ to both sides of this equivalence, we get
[TABLE]
since if an invertible U∈MN(C(Sq2n−1)) with N sufficiently large conjugates an
idempotent P over C(Sq2n−1) to an idempotent
Q, then
[TABLE]
is an invertible conjugating P1⊗P to P1⊗Q.
Now we have established all the monoid structure rules for P(C(Sq2n+1)).
□
Remark. The last part of the above proof about the monoid structure
of P(C(Sq2n+1)) can
be avoided by applying the injective monoid homomorphism ρ of the
following Corollary 2 to both sides of the equivalence relations describing
the monoid structure.
Corollary 1. All projections over C(Sq2n+1) of strictly positive rank are trivial. The cancellation law
holds for projections of rank ≥1, but fails for projections of rank [math]
in case of n>0.
Proof. The only equivalence class of projection of a fixed rank k>0
is the trivial projection [P0,k]=[⊞kI~] classified above. By counting the rank, it is clear that
if ⊞kI~ and ⊞k′I~ are stably
equivalent, then k=k′. So the cancellation law holds for projections
of rank ≥1.
On the other hand, since for any distinct pairs (j,k) and
(j′,k′) with 1≤j,j′≤n and
k,k′>0, [Pj,k]=[Pj′,k′] but
[TABLE]
the cancellation law fails for such rank-[math] projections Pj,k and
Pj′,k′.
□
Corollary 2. The monoid P(C(Sq2n+1)) is a submonoid of ∏0≤l≤nZ≥ via the injective monoid homomorphism
[TABLE]
Proof. ρ is injective since we already know that ρl’s
can distinguish the standard projections Pj,k which have been shown to
constitute the whole monoid P(C(Sq2n+1)).
□
5 Generating Projections of K0(C(CPqn))
In this section, we present a set of elementary projections over C(CPqn), whose K0-classes form a set of free
generators of the abelian group K0(C(CPqn)). We remark that a fascinating geometric construction
of free generators of K0(C(CPqn)) has been found by D’Andrea and Landi in [8].
As discussed before, by restricting to the degree-[math] part of the groupoid
Fn consisting of exactly those [(z,x,w)] with z=0, we get a subgroupoid (Fn)0 which realizes C(CPqn) as a groupoid
C*-algebra C∗((Fn)0).
Roughly speaking, (Fn)0 can be extracted
from Fn by simply ignoring or removing the z-component of
the elements [(z,x,w)]. Note that if [(0,x,w)]∈(Fn)0 and
w1=∞, then x1=0 by the defining condition on Fn. Furthermore since clearly πn(C∗((Fn)0))⊂idℓ2(Z)⊗B(ℓ2(Z≥n)), we will ignore the factor
idℓ2(Z) and view πn∣C∗((Fn)0) as a
faithful representation of C∗((Fn)0) on ℓ2(Z≥n) instead of
on ℓ2(Z×Z≥n).
In [24], by considering the closed invariant subset (Z≥n−1×{∞})/∼ (i.e. {[w]:w∈Z≥n−1×{∞}} even though Z≥n−1×{∞} is not really ∼-invariant in the unit space Z≥n of
Fn⊂Fn) and its complement
O0 in the unit space Z of (Fn)0 (and
of Fn as well), we get the following short exact sequence
[TABLE]
with (Fn)0∣O0≅(Zn⋉Zn)∣Z≥n. Thus
we get the following 6-term exact sequence
[TABLE]
By an induction on n≥1, we can establish K0(C(CPqn))≅Zn+1 and K1(C(CPqn))=0. In fact, in the case of
n=1, we have Ki(C(CPq0))=Ki(C)≅δ0iZ and hence
K0(C(CPq1))≅Z⊕Z and K1(C(CPq1))=0. For n>1, the induction hypothesis K1(C(CPqn−1))=0 and K0(C(CPqn−1))≅Zn forces
[TABLE]
and also K1(C(CPqn))=0 in
the above 6-term exact sequence.
The above induction can be refined to get the following stronger result. First
we note that
[TABLE]
with 0<j≤n is a projection in C(CPqn)⊂C(Sq2n+1), and can be identified with
[TABLE]
From now on, we view Pj,k with 0<j≤n as the latter elementary
tensor product lying in C(CPqn). On the other
hand, clearly the trivial projection P0,k of rank k over C(Sq2n+1) is also a trivial projection of rank k over
C(CPqn).
Theorem 2. The standard projections Pj,1≡(⊗jP1)⊗(⊗n−jI) over C(CPqn) with 0≤j≤n are inequivalent over
C(CPqn) and their equivalence classes (over
C(CPqn), not over C(Sq2n+1)) form a set of free generators of K0(C(CPqn))≅Zn+1.
Proof. Since Pj,1 are inequivalent over C(Sq2n+1), they are clearly inequivalent over the subalgebra
C(CPqn). Now we prove by induction on n≥1
that [Pj,1] with 0≤j≤n form a set of free
generators of K0(C(CPqn)).
For n=1, it is well-known that K(ℓ2(Z≥))+≅C(CPq1) has [P1]≡[P1,1] and
[I]≡[P0,1] as free generators of its
K0-group K0(K(ℓ2(Z≥))+)≅Z2.
For n>1, K0(K(ℓ2(Z≥n)))≅Z has [⊗nP1]≡[Pn,1] as a free generator, while by
induction hypothesis, K0(C(CPqn−1))≅Zn has [Pj,1′]≡[(⊗jP1)⊗(⊗n−1−jI)] with 0≤j≤n−1 as free generators. Now
with ν∗([Pj,1])≡ν∗([Pj,1′⊗I])=[Pj,1′] for all 0≤j≤n−1, it is easy to see from
the above 6-term exact sequence that [Pj,1] for 0≤j≤n−1 together with [Pn,1] form a set of free
generators of K0(C(CPqn))≅Zn+1.
□
It is of interest to point out that these projections Pj,1 freely
generating K0(C(CPqn)) are
actually lying inside C(CPqn)≡M1(C(CPqn))⊂M∞(C(CPqn)) and they form an
increasing finite sequence of projections.
6 Quantum line bundles over C(CPqn)
In this section, we identify the quantum line bundles Lk≡C(Sq2n+1)k of degree k over C(CPqn) with a concrete (equivalence class of)
projection described in terms of the basic projections. We remark that an
intriguing noncommutative geometric study of these line bundles in comparison
with Adam’s classical results on CPn has been successfully
accomplished by Arici, Brain, and Landi in [2]. (The degree
convention is different in the ±-sign.)
To distinguish between ordinary function product and convolution product, we
denote the groupoid C*-algebraic (convolution) multiplication of elements in
Cc(G)⊂C∗(G) by ∗, while omitting ∗ when the elements are represented as
operators or when they are multiplied together pointwise as functions on
G. We also view Cc(Fn) or
Cc((Fn)k) (also
abbreviated as Cc(Fn)k) as left
Cc(Fn)0-modules with Cc(Fn) carrying the convolution algebra structure as a
subalgebra of the groupoid C*-algebra C∗(Fn). Similarly, for a closed subset X of the unit space of
Fn, the inverse image Fn↾X of
X under the source map of Fn or its grade-k component
(Fn↾X)k≡(Fn)k↾X gives rise to a left
Cc(Fn)0-module Cc(Fn↾X) or Cc(Fn↾X)k.
For k∈Z≥, the characteristic function χBk∈Cc((Fn)0) of the compact
open set
[TABLE]
is a projection over C∗((Fn)0)≡C(CPqn) which is
represented under πn as P−k⊗(⊗n−1I),
and
[TABLE]
where Bk⊂(Fn)0 in the notation
↾Bk is canonically viewed as a subset of the unit space
of (Fn)0.
For k≤0, it is straightforward to check that
[TABLE]
well defines a bijective homeomorphism. For example, for w1=∞, we
have x1=−k on the domain side and x1+k=0 on the range side of this
map, matching the implicit constraints imposed on (Fn)k and (Fn)0. Furthermore
since any [(k,x,w)]∈(Fn)k and its image [(0,x1+k,x2,..,xn,w1−k,w2,..,wn)] share the same target
element [x+w]∈Z≥n/∼, it
induces a left Cc((Fn)0)-module isomorphism
[TABLE]
which extends to a left C(CPqn)-module
isomorphism
[TABLE]
i.e. the quantum line bundle Lk for k≤0 is the finitely generated
left projective module determined by the projection P−∣k∣⊗(⊗n−1I) over C(CPqn).
For k>0, the situation is much more complicated. We first define the closed
open set
[TABLE]
with each Cc((Fn)k,j) a
left Cc((Fn)0)-module.
Note that
[TABLE]
with χ({0}j×Z≥n−j)/∼ represented under πn as the projection (⊗jP1)⊗(⊗n−jI) over
C(CPqn).
Now the left Cc((Fn)0)-module Cc((Fn)k,j) can
be decomposed as
[TABLE]
It is straightforward to check that
[TABLE]
[TABLE]
well defines a bijective homeomorphism. For example, we are considering only
w with w1=...=wj=0<∞, while for wj+1=∞, we have
xj+1=−k−x1−⋯−xj on the domain side and −x1−⋯−xj−(xj+1+k)=0 on the range side of this map, matching
the implicit constraints imposed on (Fn)k
and (Fn)0. Furthermore since any \left[\left(k,x,w\right)\right]\ and its image under this bijection share
the same target element [x+w]∈Z≥n/∼, it induces a left Cc((Fn)0)-module isomorphism
[TABLE]
which extends to a left C(CPqn)-module
isomorphism
[TABLE]
On the other hand, for any 0≤l≤k−1,
[TABLE]
[TABLE]
well defines a bijective homeomorphism which preserves the target element
[x+w] and hence induces a left Cc((Fn)0)-module isomorphism
[TABLE]
So summarizing, we get the isomorphism relation
[TABLE]
which is recursive in the sense that the right hand side contains terms with
either k decreased or j increased. So repeated application of this
recursive expansion can lead to a direct sum of terms of the form
Cc((Fn)0,m) or the form
Cc((Fn)l,n), where
[TABLE]
while
[TABLE]
well defines a bijective homeomorphism which induces a left Cc((Fn)0)-module isomorphism
[TABLE]
extending to a left C(CPqn)-module
isomorphism
[TABLE]
Theorem 3. For n≥1, the quantum line bundle Lk≡C(Sq2n+1)k of degree k∈Z over
C(CPqn) is isomorphic to the finitely
generated projective left module over C(CPqn)
determined by the projection P−∣k∣⊗(⊗n−1I) if k≤0 (with P−0:=I understood), and the
projection
[TABLE]
if k>0, where Cjk denotes the combinatorial number (k!)/(j!(k−j)!).
Proof. Having already taken care of the case of k≤0 in the above
discussion, we only need to consider the case of k>0.
First we establish by induction on l that
[TABLE]
Indeed for l=1, (**) becomes
[TABLE]
which is the same as the established recursive relation () with j=0. For
n≥l>1, by the induction hypothesis for l−1 and the recursive relation
(), we get
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
where
[TABLE]
[TABLE]
[TABLE]
[TABLE]
and similarly
[TABLE]
Thus () holds for n≥l>1, concluding the inductive proof of ().
Now by (**) for l=n, we get
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
where again
[TABLE]
Thus Lk for k>0 is implemented by the projection
[TABLE]
□
Bibliography31
The reference list from the paper itself. Each links out to its DOI / PubMed record.
1[1] P. Ara, M. A. Moreno, and E. Pardo, Nonstable K-theory for graph algebras , Algebras and Representation Theory 10 (2007) 157–178.
2[2] F. Arici, S. Brain, and G. Landi, The Gysin sequence for quantum lens spaces , J. Noncomm. Geom. 9 (2015), 1077-1111.
3[3] F. Arici, F. D’Andrea, P.M. Hajac, and M. Tobolski, An equivariant pullback structure of trimmable graph C*-algebras , ar Xiv:1712.08010 v 3.
4[4] K. A. Bach, A cancellation problem for quantum spheres , Thesis, U. of Kansas, Lawrence, 2003.
5[5] B. Blackadar, “ K-theory for Operator Algebras ”, MSRI Publications Vol. 5,. Cambridge University Press, Cambridge, 2nd ed., 1998.
6[6] A. Connes, “ Noncommutative Geometry ”, Academic Press, New York, 1994.
7[7] R. E. Curto and P. S. Muhly, C*-algebras of multiplication operators on Bergman spaces , J. Func. Anal. 64 (1985), 315-329.
8[8] F. D’Andrea and G. Landi, Bounded and unbounded Fredholm modules for quantum projective spaces , J. K-theory 6 (2010), 231-240.